Search results for "electromagnetic transition"

showing 10 items of 31 documents

Majorana parameters of the interacting boson model of nuclear structure and their implication for 0νββ decay

2021

photonuclear reactionsnuclear spinelectromagnetic transitionsparitylifetimeswidthscollective modelspesonance reactionsneutrinoless double beta decay
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Prompt and delayed spectroscopy of 203At : Observation of a shears band and a 29/2+ isomeric state

2018

Using fusion-evaporation reactions, a gas-filled recoil separator, recoil-gating technique and recoil-isomer decay tagging technique we have extended the level scheme of 203 At ( N = 118 ) significantly. We have observed an isomeric [ τ = 14.1 ( 3 ) μ s ] state with a spin and parity of 29 / 2 + . The isomeric state is suggested to originate from the π ( h 9 / 2 ) ⊗ ∣ ∣ 202 Po ; 11 − ⟩ coupling, and it is depopulated through 286 keV E 2 and 366 keV E 3 transitions. In addition, we have observed a cascade of magnetic-dipole transitions which is suggested to be generated by the shears mechanism. peerReviewed

level densitiesnuclear spinelectromagnetic transitionsnuclear density functional theorytiheysfunktionaaliteoriaspektroskopialifetimeswidthsenergy levelsNuclear Experimentisomer decaysydinfysiikkanuclear parity
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X(5) critical-point symmetries in 138Gd

2011

International audience; The lifetimes of low-lying transitions in 138Gd have been measured using the recoil-distance Doppler-shift technique. The resultant reduced transition probabilities have been compared to X(5) critical-point calculations to assess the potential 'phase-transitional' behaviour of 138Gd. The X(5) symmetry describes the first order 'phase transition' between sphericity, U(5) and an axially deformed nuclear shape, SU(3). Although a high degree of correspondence is observed between the experimental and theoretical excitation energies, the large uncertainties of the experimental B(E2) values cannot preclude contributions from either vibrational or rotational modes of excitat…

PhysicsHistory010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]First order01 natural sciencesCritical point (mathematics)Computer Science ApplicationsEducationBohr modelSphericityKokeellinen ydinfysiikka21.10.Tg Lifetimes widths 27.60.+j 90(less-than-or-equal-to)A(less-than-or-equal-to)149 21.65.-f Nuclear matter 23.20.-g Electromagnetic transitions 21.10.Re Collective levels 21.60.Ev Collective modelssymbols.namesakeQuantum mechanics0103 physical sciencesHomogeneous spacesymbolsExperimental nuclear physics010306 general physicsHamiltonian (quantum mechanics)Axial symmetryExcitation
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Isospin symmetry in $B(E2)$ values: Coulomb excitation study of ${}^{21}$Mg

2018

The $T_z$~=~$-\frac{3}{2}$ nucleus ${}^{21}$Mg has been studied by Coulomb excitation on ${}^{196}$Pt and ${}^{110}$Pd targets. A 205.6(1)-keV $\gamma$-ray transition resulting from the Coulomb excitation of the $\frac{5}{2}^+$ ground state to the first excited $\frac{1}{2}^+$ state in ${}^{21}$Mg was observed for the first time. Coulomb excitation cross-section measurements with both targets and a measurement of the half-life of the $\frac{1}{2}^+$ state yield an adopted value of $B(E2;\frac{5}{2}^+\rightarrow\frac{1}{2}^+)$~=~13.3(4)~W.u. A new excited state at 1672(1)~keV with tentative $\frac{9}{2}^+$ assignment was also identified in ${}^{21}$Mg. This work demonstrates large difference…

electromagnetic transitionsenergy levels and level densitiesshell modelFOS: Physical sciencescollective levelscoulomb energies and analogue statesNuclear Experiment (nucl-ex)isomer decaysydinfysiikkaNuclear Experiment
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Evolution of Octupole Deformation in Radium Nuclei from Coulomb Excitation of Radioactive $^{222}$Ra and $^{228}$Ra Beams

2020

There is sparse direct experimental evidence that atomic nuclei can exhibit stable pear shapes arising from strong octupole correlations. In order to investigate the nature of octupole collectivity in radium isotopes, electric octupole ($E3$) matrix elements have been determined for transitions in $^{222,228}$Ra nuclei using the method of sub-barrier, multi-step Coulomb excitation. Beams of the radioactive radium isotopes were provided by the HIE-ISOLDE facility at CERN. The observed pattern of $E$3 matrix elements for different nuclear transitions is explained by describing $^{222}$Ra as pear-shaped with stable octupole deformation, while $^{228}$Ra behaves like an octupole vibrator.

Nuclear TheoryAtomic Physics (physics.atom-ph)Nuclear TheoryFOS: Physical sciencesnuclear structure and decaysPhysics - Atomic PhysicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)electromagnetic transitionsPhysics::Accelerator Physicscollective levelsPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)ydinfysiikkaNuclear ExperimentNuclear Experiment
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The M4 transitions of isomeric states

2015

Tässä pro gradu -tutkielmassa tutkitaan isomeeristen tilojen magneettisten M4-gammasiirtymien redusoituja matriisielementtejä. Tutkittavat siirtymät ovat venyneitä M4-siirtymiä kaksoisbeetahajoamisten massa-alueilla A=85-115 ja A=135-143. Tutkielman tarkoituksena on verrata kokeellisia ydinmatriisielementtejä kvasihiukkasmatriisielementteihin ja MQPM-teorian avulla laskettuihin matriisielementteihin. Kokeelliset matriisielementi lasketaan kokeellisesti määritettyjen arvojen avulla ja kvasihiukkas- sekä MQPM-matriisielementit määritetään tietokoneohjelmien avulla. Kokeellisten ja kvasihiukkasmatriisielementtien välinen suhde osoittautui olevan noin 0,29 ja kokeellisten ja MQPM-matriisielemen…

QRPA theoryElectromagnetic transitionsBCS theoryMQPM theorysähkömagnetisminuclear matrix elementsM4 transition
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Chirality of 135 Nd reexamined : Evidence for multiple chiral doublet bands

2019

One new pair of positive-parity chiral doublet bands have been identified in the odd-A nucleus 135Nd which together with the previously reported negative-parity chiral doublet bands constitute a third case of multiple chiral doublet (MχD) bands in the A ≈ 130 mass region. The properties of the MχD bands are well reproduced by constrained covariant density functional theory and particle rotor model calculations. The newly observed MχD bands in 135Nd represents an important milestone in supporting the existence of MχD in nuclei. peerReviewed

electromagnetic transitionsHigh Energy Physics::Phenomenologycollective levelscollective modelsydinfysiikka
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Evidence of chiral bands in even-even nuclei

2018

Evidence for chiral doublet bands has been observed for the first time in the even-even nucleus 136 Nd . One chiral band was firmly established. Four other candidates for chiral bands were also identified, which can contribute to the realization of the multiple pairs of chiral doublet bands ( M χ D ) phenomenon. The observed bands are investigated by the constrained and tilted axis cranking covariant density functional theory (TAC-CDFT). Possible configurations have been explored. The experimental energy spectra, angular momenta, and B ( M 1 ) / B ( E 2 ) values for the assigned configurations are globally reproduced by TAC-CDFT. Calculated results support the chiral interpretation of the o…

Physicslevel densitiesta114010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::Phenomenology[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesMolecular physicsnuclear structure and decaysmedicine.anatomical_structureelectromagnetic transitionsPhysical Sciences0103 physical sciencesmedicineFysikcollective levelsenergy levels010306 general physicsNucleus
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Restoring the valence-shell stabilization in 140Nd

2020

A projectile Coulomb-excitation experiment was performed at the radioactive-ion beam facility HIE-ISOLDE at CERN to obtain $E2$ and $M1$ transition matrix elements of $^{140}$Nd using the multistep Coulomb-excitation code GOSIA. The absolute $M1$ strengths, $\textrm{B}(M1;2^+_2→2^+_1)=0.033(8)μ^2_N,\textrm{B}(M1;2^+_3→2^+_1)=0.26^{+0.11}_{−0.10}μ^2_N$, and $\textrm{B}(M1;2^+_4→2^+_1)<0.04μ^2_{\textrm{N}}$, identify the $2^+_3$ state as the main fragment of the one-quadrupole-phonon proton-neutron mixed-symmetry state of $^{140}$Nd. The degree of F-spin mixing in $^{140}$Nd was quantified with the determination of the mixing matrix element $V_{\textrm{F−mix}}<7^{+13}_{−7}$keV.

electromagnetic transitionsNuclear Physics - Experimentcollective levelsydinfysiikkanuclear structure and decays
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Decay of a 19− isomeric state in 156Lu

2018

A multiparticle spin-trap isomeric state having a half-life of 179(4) ns and lying 2601 keV above the yrast 10 + state in 156 Lu has been discovered. The 156 Lu nuclei were produced by bombarding isotopically enriched 106 Cd targets with beams of 58 Ni ions, separated in flight using the gas-filled separator RITU and their decays were measured using the GREAT spectrometer. Analysis of the main decay path that populates yrast states observed previously suggests a spin-parity assignment of 19 − for the isomeric state, which is consistent with isomeric states identified in the N = 85 isotones. Comparison with other decay paths in 156 Lu indicates that the [ π h − 1 11 / 2 ⊗ ν h 9 / 2 ] 10 + st…

electromagnetic transitionsisomer decaysydinfysiikkanuclear structure and decays
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